Frequency change indicator



Aug. 28, 1951 v Filed Oct. 11, 1947 T. E. LYNCH 2,566,222

FREQUENCY CHANGE INDICATOR 4 Sheets-Sheet 2 A ORNEY 1951 T. E. LYNCH 2,566,222

FREQUENCY CHANGE INDICATOR Filed Oct. 11, 1947 4 Sheets-Sheet :5

SOURCE RECORDER AAA All

JNVENTOR. THOMAS E. LYNCH Aug. 28, 1951 T. E. LYNCH 2,565,222

FREQUENCY CHANGE INDICATOR Filed Oct. 11, 1947 4.Sheets-$heet 4 INVENTOR; THSMAS E. LYNCH Patented Aug. 28, 1951 FREQUENCY CHANGE INDICATOR Thomas E. Lynch, Cleveland, Ohio, assignor to The Brush Development Company, Cleveland,

Ohio, a corporation of Ohio Application-October 11, 1947, SerialNo. 779,369

8 Claims.

The present invention relates to an apparatus for providing an indication of frequency changes of a wave signal. While the invention is of gen- 'eral application, itis of, particularutility in providing indications of frequency changes which are due to variations in the speed of a mechanical drive system which is utilized to generate the signal the variations of frequency of which are measured.

There are many uses for an apparatus which will provide an indication of small frequency changes of a wave signal. Thus, in some cases, it has been the practice to utilize a tone wheel to "generate an alternating potential, the frequency of which depends upon :amechanical .sys tem driving the tone wheel. In some cases, the frequency of the signal generated by the tone wheel has been utilized to provide an indication of the speed of the mechanical system and of variations in this speed due to various undesired deficiencies in'the gearing, bearings, shafts, driv ing motor, etc. Perhaps the most important use, of apparatus for providing indications of frequency changes, of a wave signal .of the type under consideration, relates to the checking of the drive mechanism of sound-reproducing systems.

In a sound-recording and reproducing system, if a sound of exactly constant frequency is recorded and thereafter reproduced it is generally found that, even though the average frequency of the reproduced signal corresponds exactly to the frequency of the sound which was originally recorded, variations-or "imperfections .in the gears, bearings, shafts "and motor cause certain changes or variations in .the frequency of the reproduced such circumstances, the frequency of the reproduced signal increases and decreases in synchronism with the rotation of the gear which is defective. of the reproduced signal, or of frequency changes thereof, provides a good check upon this feature of the mechanical drive system. It is apparent, therefore, that a considerable knowledge of the accuracy of the drive system can 'be obtained Thus, a measurement of the frequency from an analysisof the frequency components in the reproduced output signal.

The rates of frequency variations of the reproduced signal which are here 'underconsideration and which are .most troublesome 'lie within the range of to 200 cycles per second. The low-frequency components in this range of signals are generally called wow components by sound engineers; whereas, the .high frequency components within this range aregenerallycalled flutter components. Components of either of these types are very annoying in a reproduced sound signal. While an elaborate recording apparatus may sometimes be utilizedto record sound on a record medium, and thus "provide a recording which is substantially free from undesirable components of the typehere-under consideration, it is generally true that the reproducing apparatus is much less elaborate and is likely to be the most frequent cause of trouble. In the manufacture of sound-signal reproducing apparatus, therefore, it is of particular importance to have available :an apparatus which provides a ready :and easily calibrated indication of deficiencies in the mechanical drive system of the apparatus.

The apparatus which has previously been used for checking mechanical drivesystems has generally had the .defectslof a low sensitivity, critical and frequent calibration requirements, the requirement of a carefully controlled carrier signal, faulty results due to amplitude modulation of a carrier'signal used in the system, restricted frequency range, the requirement of elaborate additional equipment, and difficulty due to starting transients in the system. vIt would :be very desirable, therefore, to provide an apparatus of the type under consideration and .in which all of these defects are eliminated.

It is, therefore, an object of the invention to provide an apparatus for indicating frequency changes of a wave signal which is not subject to one or more of the above-mentioned defects of prior such'apparatus.

It is an object of the invention .to :provide an improved apparatus .for indicating frequency changes of a wavesignal.

It is an object of the invention .to ,provide an apparatus for indicating frequency .changes of a wave signal and which .can be accurately .calibrated in theabsence of .known variations in the frequency of the signal.

It is still another object of the invention .to provide an improved apparatus, for indicating frequency changes .of a waveslgnal, which has 3 a substantially linear output characteristic over its entire range of operation.

In accordance with the invention, an apparatus for providing an indication of frequency changes of a first wave signal comprises means for deriving sharp electrical pulses having relative spacings dependent upon the intercepts of this wave signal. The apparatus also includes means dependent upon the sharp pulses for de'-= riving a second wave signal having only separate portions corresponding respectively to each of the sharp pulses and having identical average values in each of these portions. The apparatus also comprises means for deriving a third signal varying in accordance with the average value, over a relatively short time interval, of the frequency components of the above-mentioned second signal which have a period less than a predetermined time substantially greater than the above-mentioned short time interval. There is also provided means for utilizing the above-mentioned third signal to provide indications of changes of frequency of the above-mentioned first wave signal.

For a better understanding of the present invention together with other and further objects thereof, reference is had to the following de scription taken in connection with the accon1- panying drawings, and its scope will be pointed out in the appended claims.

Fig. 1 of the drawings is a block diagram of an apparatus in accordance with the invention for providing indications of frequency changes of a wave signal; Fig. 2 comprises curves utilized to describe operation of the apparatus of Fig. l; and Figs. 3, 4, and 5, respectively, illustrate certain specific circuits which may be used in the units I3, I4, and I of the apparatus of Fig. 1.

Referring now more particularly to Fig. 1, an apparatus is there shown for providing an indication of frequency changes of a first wave signal. These frequency changes may, for example, be frequency changes in the wave signal of an oscillator II), as recorded and thereafter reproduced by a device under test I l. A two-position switch I2 is provided for connecting device H to oscillator In so that the signal output of the oscillator is recorded and thereafter for connecting unit II to components of the system utilized to rate portions corresponding respectively to each of the sharp pulses and having identical average values in each of its portions. Specifically, the system is preferably such that a rectangular pulse of pre-determined duration is provided in pulse shaper I4 for each sharp pulse supplied thereto from pulse former I3. Such a signal with rectangular pulses thus has only separate portions,

namely, the portions from the beginning of one pulse to the beginning of a second pulse, corresponding respectively to each of the sharp pulses derived from unit I3 and each of these portions has an identical average value.

A frequency selector I5 is coupled to the output circuit of pulse shaper I l and is effect ve t 4 select only those components of the signal output of pulse shaper [4 which have a period less than a predetermined time, for example, less than two seconds. The frequency components present in the output circuit of unit I5, namely, the frequency components of the second signal provided by unit I5 which have a period less than a predetermined time which in the Specific example chosen is a time of two seconds, are averaged over a relatively short time interval, for example /200 of a second, by an integrator I 5.

An adjustable-gain amplifier i7 is coupled to the output circuit of integrator I6 and the output circuit of amplifier I? is supplied to an input circuit of a motor driven recorder I8 through a three-position switch I9. The switch I9 is so connected that the signal input to recorder I8 can be taken from a frequency selector 29, for one position of switch l9, can be taken directly for asecond position of switch. I9 as shown in the drawing, and can be taken through another frequency selector 2| for a third position of switch I9. The frequency selector 20 is effective to select all frequency components of the output signal of amplifier I1 within the frequency range of to 10 cycles. The frequency selector 2| is effec' tive to select all frequency components of the output signal of the amplifierl? within the ire-- quency range of from 10 to 200 cycles.

A 60-cycle source 23 is provided for driving a motor associated with recorder Iii. In order to provide an easily operated calibration arrange ment for the apparatus of Fig. l, a two-position switch 25 is provided between units I4 and I5. In one of its positions, the switch 25 connects the output circuit of pulse shaper I4 to the input circuit of frequency selector I5 while, in its other position, the switch 25 is effective to couple an output circuit of the source 23 to the input circuit of frequency selector I5. A voltmeter 25 is coupled across the input circuit of frequency selector I5.

In considering the operation of the apparatus of Fig. 1, reference is made to the curves of Fig. 2 which illustrates certain of the wave forms which are present in the system during operation.

' Thus for example, the output signal of oscillator IIi during an interval of time 151 to 152 may be as illustrated by the curve A. It will furthermore be assumed that device II is a magnetic recorder and reproducer. Thus, when the device I I is connected to the oscillator It], the output of oscillator In is recorded in the device I I. When the switch I2 is operated to connect the device II to the pulse former I3, it will be assumed that the recorded signal is reproduced in the device I I and supplied to pulse former I3. Under these conditions, the reproduced signal should have the exact wave form of curve A of Fig. 2. However. as explained above, a reproduced signal does not usually have this exact wave form due to minute variations in speed of the mechanical drive system involved which may cause the reproduced signal to have a frequency which is either too high or too low during short intervals of time even though its average value is correct. Also, while not important in the case under consideration, the amplitude of the reproduced signal may have undesirable variations. Thus, the curve B of Fig. 2 illustrates what may be the wave form of the reproduced signal of the device II during a pre-determined short time interval 3 to in if, during this interval, the reproduced signal has a frequency which is too high. Conversely, the wave form of curve C may illustrate the wave o m-ma 5 mm of the signal output or {device Iii durin an interval $5 to to whenthe frequency iUf reproduced signal is too low.

Thezpulse former i3 is effective *to derivexshan'p negative pulses having relative spacings depend ing'upon th'e intercepts of the wave-signal *input thereto. The sharp pulses which are thus adeveloped hy :pulse former P3 during the rmtervalls tr-tz, via-t4, and ts-is are thus represented by the curves A1, and I31, respectively, of Fig.

' The means "for deriving above-mentioned :seoond wavesignal comprises the lpulsestraper t4 --which responsive to eachlpulse of -.curves A1,

*B1, and-C1, for deriving a' rectangular pulse ofpredetermined duration. These pulses of rectangular wave form are illustrated by the curves A2, m, and respectively.

The unit I B is effective to select the frequency components above "V cyc l e per secondof the pulse signals A2, B2, and 02, while the integrator I B is eflective to integ-ra' te the selected components over 25 second "intervals. The order of the operations performed by units lli "and it is uni-m- 'por tant and the "curves of Fig. illustrate the case where the integration of unit Hi is provided before frequency selector I 5 is effective. "Thus,

the integration of the wave forms of curves A2,

B2, and C2, rt-zsp'ectively, over "a pre-determined time interval which may be second, provides a varying unidirectional output as illustrated by thecurves .Ac, B3, and C3, respectively. When,

"advantageously after further amplification, the

very low-frequency "components (including tlre direct-current component) are eliminated from the signal which includes portions represented V by curves A3, B3, "and C3, the signal stabilizes itself about its alternating-current axis, thus providing anoutput signal which includes corresponding amplified portions as represented by curves A4, B4, and C4.

*The signal having portions represented 'by curves A4, B4, and 04 is amplified in thexadjustable-"gain amplifier H and "supplied "to the recorder Ill. The recorder 1'8 tmay be any motordriven recorder of the'pap'er tape typeandis'thus effective, when the "switch {-9 is in the "position shown, to plot 'acurve of the type illustrated .in

*Fig. "2 and including the portions A4, B4, and C4.

"The amplitude of this curve indicates the extent "of frequency changes "of the reproduced "signal derived from "the output circuit of the device under test I-l. Since the speed (of travel of the paper tape in the recorder "is known, it follows that the rate of these frequency changes also is indicated.

in many mechanical-drive systems, the components of -'frequency changes having rates of change within the range of 1 /2 to cycles are of particular importance. As stated above, these "are "called Wow components by sound engineers and the recorder I8 is effective to plot such frequency components when the switch I9 'is op- B the ilmowniinrterms of .I-roguency deviation 10f ifii naloutput .of iherlevicewunder test M. A prerferred-scalihration' pmicedm'e will therefore he described. in order to reflect the calibration, a signal output .of :lmown frequency from the :device His ifirst applied through switch .12. to the input circuit of unit 13 and the average voltage present at the input rcircnit of frequency selector has determined T-by reference to meter 2.6. This represents the voltage/present at the input -cuitcof lsliiorasignal of pro-determinedirequencyapplieii to the :system. ,Since, :inthe noroperation-1rd :the instrument, lthfi "voltage at the input tcircu'rtrrof unit 15 varies linearly with frequency, it is known that a given change of the frequency of the :input :signal will produce a like average voltage change .at the input circuit of unit 45. .Also, :since the portion of the instru- 311E111, following circuit [4 :is operated only by "voltage changes, it :is :sufficient to adjust the response of recorder 21:8 to provide the desired deflection tfornny known voltage change at the input circuit of x-uni-t CI'5. The frequency of the calibrating :signal for this portion of the instrument "is not of importance 'so long as this .freenemy is within the range of frequency response of this portion :of the instrument including the recorder 18. Accordingly, therefore, the switch 255 operated so that the :GO-cycle souroeifl is connected :directly to the :input circuit of :frequency rselector l5 and the amplitude of the 60- "cycle voltage so applied .is adjusted to he .equal to the above-mentioned lmown change in "volt- :age. This zoo-cycle signal :is transmittedthrough the system andrecorded by the recorder 1.8. The gain of amplifier 11 is then adjusted .to provide "the amplitude of recording I011 the recorder 18 desired. Under these conditions, the instrument is therefore calibrated :so that frequency variations corresponding to a known percentage change of the signal output of the device under test -I l, which in turn are effective to :produce -cor-responding voltage variations 10f the signal input to unit =|5, also produce this desired deflection on the recorder I 8. Also, since the characteristic of the unit is a linear one, greater or smaller variations in the frequency of the signal output or the device under test ll produce .cor- "respondin'gly greater or smaller amplitudes of recording by the recorder 18.

Ilhenrfi'ts -of Fig. '1,Wlth the exception .of pulse former 'l 3,'pulse shaper l-4', and frequency selector l5 are well "understood by those skilled 'in the art, rendering a detailed description :unnecessary. ispecific circuits which have been found to lhavepar ticulariutility in units l5, l4, and 1:5 will be described hereinafter. Thus, Fig. 3 there is illustrated a :c'ircuit 'uihich may be utilized ee the pulse former L3. This circuit comprises a transformer on connected in lthB :circuit of a Tull-wave rectifier, including :a r10uble-diode vacuum tube 3 l' and an output resistor The input circuit or a pentode vacuum tulce 33 is coupled across the resistor The output circuit of "tube 33 includes a load resistor 84 and a coupling network, including a series condenser '35 and a shunt resistor 35 across which the output'voltage of the unit isderived. A shunt oondenser 37 "and ashunt resistor 38 are'included in theiscreencircuit of tube 33 anda suitale'le 'op- 'erating voltage is supplied to the screen grid of the tube through a'resistor 38 from the source of unidirectional operating voltage for' the tubegindicated as l-EB. 1h considering theoperation of thecircuit-dfWig.39ft will 'beeeen that-the-tube 31 acts as a full-wave rectifier'to provide half sine waves of negative polarity across resistor 32; The voltage supplied to the grid of tube 33 thus has a high negative value so that, throughout most of the cycle, the input electrode thereof has a negative potential applied thereto which is sufiicient to maintain the tube non-conductive. However, when the input signal to tube 33 approaches the value of zero potential, as it does on the intercepts of alternating potential applied to the input circuit of transformer 3|], the tube 33 becomes conductive to produce sharp negative pulses in the output circuit, these sharpnegative pulses being as illustrated in curves A1, B1, and

C1 of Fig. 2.

The pulse shaper |4 may be provided by a circuit arrangement in accordance with that illustrated in Fig. i. In order to derive the pulses of curves A2, B2, and C2 of Fig. 2, a trigger circuit is utilized which includes pentode tubes 40 and 4| having a common cathode resistor 42 and having cross connections between the anode of each tube and a control electrode of the other tube to provide a well-known trigger action. Separate load resistors 44 and A are provided, respectively, for the tubes 46 and 4|, 2. common load resistor 46 also being provided. A stabilizing diode 41 is connected between a signal-input electrode of tube 49 and ground in order to stabilize the bases of the sharp pulses from unit l3 of Fig. 1 at the zero potential level. An output signal is derived from the trigger circuit by means of a connection to the anode of tube 40, this signal being applied to the input circuit of a triode 49, through a coupling condenser 56. Series-connected resistors 5! and 52 are provided in the cathode circuit of tube 49 and a resistor 53 is connected between the control electrode of tube 49 and the common junction of resistors 5| and 52. A signal output is derived from the series-connected resistors 5| and 52 and applied, through a condenser 54 and resistor 55, to the input circuit of a short-circuited delay line. This delay line includes series inductance elements L and shunt capacitance elements C. A terminating inductor 58 is connected across thelast shunt condenser 56 of the delay line and a matching impedance termination is provided at 'the input terminals of the delay line. This termination comprises a shunt resistor 59 and a combination of an inductor 6i! and a condenser 6|. The first shunt condenser of the delay line is designated by the reference numeral 57.

The signal present at the input terminal of the delay line is also amplified in a triode vacuum tube 64, the tube 64 having a cathode resistor 55 and an anode resistor 65. An output signal is coupled from the anode circuit of tube 64 to the input circuit of a limiter tube 63 through a coupling network including a shunt resistor 69 and a series condenser l0. A parallel-connected resistor H and condenser E? are included in the cathode circuit of tube 68. Tube 63 is also provided with a load resistor is and an output potential is derived from the anode circuit of this tube and applied to a control grid of tube 4|, through a coupling network including a series condenser 14 and a shunt resistor 15. A stabilizing diode T! is provided between the input electrode of tube 4| and ground. The cathode of tube 68 is connected to the unidirectional source of supply for the system, indicated +B, through a resistor 19.

The output signal of the arrangement of Fig. 4 is derived at a terminal 80 through a vacuum tube 8| having an input circuit connected through a resistor 82 to the common terminal of condenser 54 and resistor 55. A cathode resistor 83 is provided for tube 8| and a load resistor 84 is provided for the tube. A meter 85 is connected across the load resistor 84 through a resistor 86. A stabilizing diode 81 is provided between the common junction of condenser '54 and resistor 82 and ground.

In considering the operation of the circuit of Fig. 4 it will be seen that the tubes 40 and 4| are cross-connected to provide a well-known type of trigger circuit. The circuit elements are so chosen that tube 40 is normally conductive in the absence of a negative pulse output from the sharp pulse former l3. The diode 4'! is effective to stabilize the bases of the sharp pulses of curves A1, B1, and C1 at the zero potential level. The arrival of one of the sharp pulses, therefore, is effective to cause tube 4| to become conductive. The pulse, which is present across load resistor 44 under these conditions, is translated by tube 49 and applied, through the coupling condenser 54 and resistor 55 to the input circuit of the delay line. This pulse travels down the delay line, is reflected and reversed in polarity, and returns to the input terminal of the delay line after a pre-determined time interval which depends upon the relay inherent in the circuit. It is this delay which is the main factor in controlling the duration of the pulses which are generated in the output circuit of the arrangement of Fig. 4. The round-trip time of the delayline is preferably about 200 micro-seconds. The tube 81 is eii'ective to stabilize the bases of the generated pulses at the zero-potential level.

The entire signal present-at the input circuit of the delay line is also applied to the input circuit of tube 64. The signal input to tube 64 is amplified in the tube and difierentiated in the couplin circuit, including condenser 18 and resistor 69, so that the reflected pulse derived from the delay line is effective to provide a positive sharp pulse in the input circuit of tube 68. This positive pulse is amplified and reversed in polarity by tube 68 and is thereafter applied, through the coupling condenser 14, to the first control electrode of the tube 4|. The negative pulse thus applied to the control electrode of the tube 4| has the efiect of operating the tube to cut off and, due to the cross-connection between the tubes 40 and 4|, the tube 4|! is thereby caused to be returned to its original, or conductive, state. The diode 11 is utilized to stabilize the signal input to tube 4| at the tips of the pulses. .Thus a further step voltage is applied to the input circuit of tube 49 when the tube 49 again becomes conductive. The input to tube 8|, therefore, includes the original step voltage of positive polarity, due to tube 40 becoming non-conductive by the original application of a sharp pulse thereto from the pulse former l3, and also includes the step of negative polarity due to the return of tube 40 to its normal or conductive condition in the manner described above. These two step voltages, with polarity reversal in the circuit of tube 8|, constitute the output signal of the system which is derived at terminal as. This output signal includes one pulse for each of the sharp pulses derived from pulse former 3 of Fig. 1, these pulses being of a precise duration determined primarily by the delay line of Fig. 4, the pulses being as illustrated by the curves A2, B2, and C2 of Fig. 2.

the integrator it of Fig. l.

ihefrequency selector is illustrated. in Fig. 5; Essentially, this comprises a network including a condenser 90 in series with which areconnected resistors 9|, 92; and 93 The input terminal for this unit is indicated by the reference numeral 81 and the output terminal: is incheated by the reference numeral 94.

Inasmuchas there is a sharp transient in the system of Fig. 1 when the apparatus is first placed in operation, it is desirable to provide some arrangement for preventing this transient from being applied through the system. There-. fore, a relay 95 is preferably provided having normally closed contacts 96 which are effective to short-circuit the resistors 92 and 93. This short-circuit is removed from the system when the relay 95 is energized and, in order to provide an automatic operation, the relay 196 is energized by the signal input to terminals 8? through vacuum tubes 91, 98, and 99. The purpose of this circuit is to cause relay 95 to be energized after about one second delay, when a signal input is present at terminal 81, and to be (ls-energized immediately when the signal input to terminal 81 is interrupted. Tube 98 is a diode having its anode connected to the grid of the tube 99 and its cathode connected to the cathode of tube 91. The parallel combination of a resistor I90 and condenser llll is included in the cathode circuit of tube 91, the anode and control electrode of tube 91 being connected together so that the tube operates as a diode. A resistor I9! is connected across the diode 98 and the anode of tube 98 iscoupled to groundthrough a condenser 193. A cathode resistor lMis provided for tube 99, its cathode being coupled to the source of operating potential for the system, indicated +B, through a resistor I05.

In considering the operation of the circuit of Fig. 5, it will be seen that, when relay 95 is deenergized, the time constant of the frequency selector, including the condenser 99; and its series resistance, is small due to the fact that resistors 92 and 93 are short-circuited. This small time constant allows the condenser 99 to charge quickly and the effective short circuit on terminal 94 prevents transients from being coupled to After a short time, however, the relay 95 is energized to provide the normal operation which is described above. Preferably, also, the relay 95 includes a normally open set of contacts I96 which are included in the circuit connecting the motor drive of the recorder I8 to the GO-cycle power source 23 of Fig. 1. This assures that the motor of the recorder is not driven except during those intervals when a signal is to be recorded.

While the applicant does not wish to be limited to any particular circuit values, there follows a list of certain values which have been found to be particularly effective in the circuits of Figs. 4 and 5.

Tubes 40 and Ill-type 6SJ7 Tubes 41, 11, 81, 98type 6AL5 Resistor 42-680 ohms Resistors 44 and 45- -33 kilohms Resistor 69-1 megohm Resistor 9l470 kilohms Resistor 92-470 kilohms Resistor 939 megohms Inductors L33 millihenrys with approximately 7 millihenrys between adjacent coils Inductor 58-8 millihenrys Condenser C-0.004 microfarad prising:

10 Condenser 56-0.005. microi'arad Condenser. 51-0 .003 microfarad; Condenser 10-25. micro microfarads Condenser 99--0.1 microfarad Source of uni-directional operating potentialv for the tubes (+B)-3,00. volts While there have been described what are at. present considered to be the piers-1 a; e" "bgi'di-i mer ts of; this invention, it will" be' obv ous to hose; s ed n t r th a i es pa e as modifications may be made therein without defartin it m, the i n; and s he or aimed in the appended claims to cover all such han es. and liiiq t qs a far i ih i ue. irit d Scope of h eve in I cla m s m i nt sm 1. An apparatus forproviding an indication of e uenc c an o rst w 'ia i prisi means for deriving sharp electri'cal pulses having relative spacings dependent upon the, int r of s W ve ae i me t as; stud nt 29 s d. sh pulses 6 'i second wave signal having only separate per iqn eqrr p ndi s re pe ve is each if said. sharp pulses and having identical averagevalues in each of said portions; means for deriving a third signal varying in accordance "with the average value, over a relatively short time inter l h ire en mp n nts i as s nd wave signal having a period less than a predee ined time s ant a l srsai than aid sh r inte v an mea s r iliz aidi ird signal to provide indications of changes oi frequency oi said first wave signal.

2. An apparatus for providing an indication of frequency changes of a first wave signal'comprising: means for deriving sharp electrical pulses having relative spacings dependent upon the intercepts of said wave signal; 'meansd pendent upon each of said sharp pulses for deriving a rectangular pulse of predetermined duration to provide a second wave signal; means for deriving a third signal varying in accordance with the average value, over a relatively short time interval, of the frequency components of said second wave signal having a period substan-; tially less than a predetermined time substantially greater than said short interval; and means for utilizing said third signal to provide indica;

tions of changes of frequencies of said first wave signal.

3. An apparatus for providing an indication of frequency changes of a first wave signal commeans for deriving sharp electrical pulses having relative spacings dependent upon the intercepts of said wave signal; means dependent upon said sharp pulses for derivingations corresponding respectively to each of-said sharp pulses and having identical average values in each of said portions; means for deriving the frequency components of said second wave signal which have a period less than a predetermined time; means for integrating said frequency components over an interval of time which is short with respect to said predetermined time to provide a third wave signal; and means for utilizing said third signal to provide indications of changes of frequency of said first wave signal.

4. An apparatus for providing an indication of frequency changes of a first wave signal comprising: means for deriving sharp electrical pulses having relative spacings dependent upon 15 the intercepts of said wave signal; means dependent upon said sharp pulses for deriving a second wave signal having only separate portions corresponding respectively to each of said sharp pulses and having an identical average value in each of said portions; a resistor condenser network for deriving the frequency components of said second wave signal which have a period less than a predetermined time; means for integrating said frequency components over an interval of time which is short with respect to said predetermined time to provide a third wave signal; and means for utilizing said third signal to provide indications of changes of frequency of said first wave signal.

5. An apparatus for providing an indication of frequency changes of a first wave signal comprising: means for deriving sharp electrical pulses having relative spacings dependent upon the intercepts of saidywave signal; means dependent upon said sharp pulses for deriving a second wave signal having only separate portions corresponding respectively to each of said sharp pulses and having identical average values in each of said portions; means for deriving a third signal varying in accordance with the average value, over a relatively short time interval, of the frequency components of said second wave signal having a period less than a predetermined time substantially greater than said short interval; an adjustable amplifier for amplifying said third signal; and'means for utilizing said amplified third signal to provide indications of changes of frequency of said first wave signal.

6. An apparatus for providing an indication of frequency changes of a first wave signal comprising: means for deriving sharp electrical pulses having relative spacings dependent upon the intercepts of said wave signal; means dependent upon said sharp pulses for deriving a second wave signal having only separate portions corresponding respectively to each of said sharp pulses and having identical average values in each of said portions; means for deriving a third signal varying in accordance with the average value, over a relatively short time interval, of the frequency components of said second wave signal having a period less than a predetermined time substantially greater than said short interval; means 7 including an adjustable-gain amplifier for utilizing said third signal to provide indications of changes of frequency of said first wave signal; a calibrating alternating-potential source having a period between said above-mentioned time intervals; means for measuring the average value of said second wave signal for a predetermined frequency of said first wave signal; means for applying a potential from said source, which is equal to a predetermined portion of said last-named average value, to said means forrderiving said third signal; and means for adjusting the gain of said amplifier :toprovide a predetermined indication in "response to said applied potential, therebyto calibrate said indications for all changes of frequency of saidv pendent upon said sharp pulses for deriving a.

second Wave signal having only separate portions corresponding respectively to each of said sharp pulses and having identical average values in each of said portions; means for deriving a third signal varying in accordance with the average value, over a relatively short time interval, of the frequency components of saidsecond wave signal having a period less than a predetermined time substantially greater than said short interval; a recorder; and means for utilizing said third signal to actuate said recorder to provide a record of changes of frequency of said first Wave signal. I g

8. An apparatus for providing an indication of frequency changes of a first wave signal comprising: means for deriving sharp electrical pulses having relative spacings dependent upon the intercepts of said wave signal; means dependent upon said sharp pulses for deriving a second wave signal having only separate portions corresponding respectively to each of said sharp pulses and having identical average values in each of said portions; means for deriving a third signal varying in accordance with the average value, over a relatively short time interval, of the frequency components of said second wave signal having a period less than a predetermined time substantially greater than said short interval; means for selecting predetermined frequency components of said third signal and for utilizing the selected components to provide indications of changes of frequency of said first Wave signal. I r I THOMAS E. LYNCH.

REFERENCES CITED The following references are of record in the file of this patent:

UNITED STATES PATENTS Wilbur -1 Dec. 26, 1944 

